Quantum measurement | Inequalities

CHSH inequality

In physics, the CHSH inequality can be used in the proof of Bell's theorem, which states that certain consequences of entanglement in quantum mechanics can not be reproduced by local hidden-variable theories. Experimental verification of the inequality being violated is seen as confirmation that nature cannot be described by such theories. CHSH stands for John Clauser, Michael Horne, Abner Shimony, and , who described it in a much-cited paper published in 1969. They derived the CHSH inequality, which, as with John Stewart Bell's original inequality, is a constraint on the statistical occurrence of "coincidences" in a Bell test which is necessarily true if there exist underlying local hidden variables, an assumption that is sometimes termed local realism. It is in fact the case that the inequality is routinely violated by modern experiments in quantum mechanics. (Wikipedia).

CHSH inequality
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Qubit | Tsirelson's bound | Determinism | Pauli matrices | Beryllium | Correlation does not imply causation | Bell's theorem | Density matrix | Bell state | Quantum correlation | Leggett–Garg inequality | Nitrogen-vacancy center | Phase qubit | Local hidden-variable theory | Quantum key distribution | Quantum game theory | Bell test | Quantum entanglement | Triangle inequality